2017
DOI: 10.1021/acs.jctc.7b00998
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Fermionic Statistics in the Strongly Correlated Limit of Density Functional Theory

Abstract: Exact pieces of information on the adiabatic connection integrand, Wλ[ρ], which allows evaluation of the exchange-correlation energy of Kohn–Sham density functional theory, can be extracted from the leading terms in the strong coupling limit (λ → ∞, where λ is the strength of the electron–electron interaction). In this work, we first compare the theoretical prediction for the two leading terms in the strong coupling limit with data obtained via numerical implementation of the exact Levy functional in the simpl… Show more

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Cited by 28 publications
(68 citation statements)
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“…In this case the SCE total energy E 0,SCE N =2 of section 2.2 is equal to where the right-hand side is the value of the SCE potential energy on the manifold parametrized by the co-motion function. This value is a degenerate minimum, meaning that we can evaluate it at any point lying on the manifold, such as for | r | → ∞ (for a nice illustration of the degenerate minimum of the SCE potential energy, the interested reader is addressed to Figure 1 of ref ( 57 )). When | r | → ∞, the potential v Hxc SCE ( r ) is gauged to go to zero.…”
Section: Different Types Of Response Potentials: V mentioning
confidence: 99%
“…In this case the SCE total energy E 0,SCE N =2 of section 2.2 is equal to where the right-hand side is the value of the SCE potential energy on the manifold parametrized by the co-motion function. This value is a degenerate minimum, meaning that we can evaluate it at any point lying on the manifold, such as for | r | → ∞ (for a nice illustration of the degenerate minimum of the SCE potential energy, the interested reader is addressed to Figure 1 of ref ( 57 )). When | r | → ∞, the potential v Hxc SCE ( r ) is gauged to go to zero.…”
Section: Different Types Of Response Potentials: V mentioning
confidence: 99%
“…Another possibility is to construct approximate natural orbitals, which are eigenfunctions of single-particle Hamiltonians with a local effective-potential. 20 , 21 On the DFT side, besides changing the auxiliary system for the KS construction, 22 24 a possible way out is to include the kinetic-energy density as a basic functional variable along with the density, simplifying the modeling of the exchange-correlation potentials because they will not include any more kinetic-energy contributions. This however implies that an additional auxiliary potential, which couples to the kinetic-energy density, has to be introduced.…”
Section: Introductionmentioning
confidence: 99%
“…The corresponding eigenvectors induce a set of curvilinear coordinates u µ in terms of whichĤ λ can be expanded [18,20].…”
Section: B Zero Point Energymentioning
confidence: 99%
“…The first subleading term for SCE-type solutions introduces kinetic energy in the form of zero-point oscillations (ZPE). It has been first evaluated in 2009 [18] and received numerical confirmations only recently [19,20]. Little is known yet on the third leading term, for which scaling arguments suggest it to be of purely kinetic na-ture [18,21].…”
Section: Introductionmentioning
confidence: 99%